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NEET PHYSICSMedium

Two pith balls carrying equal charges are suspended from a common point by strings of equal length, the equilibrium separation between them is r (as shown in Fig. I). Now, as shown in Fig. II, the strings are rigidly clamped at half the height. The equilibrium separation between the balls now becomes:

A

r / ∛2

B

r / √2

C

2r / 3

D

none of the above

Step-by-Step Solution

At equilibrium, the electrostatic repulsive force (FeF_e) is balanced by the component of gravity acting along the tangent of the arc. For small angles θ\theta, the condition for equilibrium is tanθ=Femg\tan \theta = \frac{F_e}{mg}.

  1. Geometry: From the figure, tanθsinθ=r/2y=r2y\tan \theta \approx \sin \theta = \frac{r/2}{y} = \frac{r}{2y}, where yy is the vertical distance from the point of suspension to the line joining the balls.
  2. Force Equation: Substituting Coulomb's law (Fe=kq2r2F_e = \frac{kq^2}{r^2}), we get kq2r2mg=r2y\frac{kq^2}{r^2 mg} = \frac{r}{2y}.
  3. Proportionality: Rearranging the terms, r3yr^3 \propto y.
  4. New Condition: When clamped at half height, the new vertical distance is y=y/2y' = y/2. Let the new separation be rr'.
  5. Calculation: (r)3r3=yy=12    r=r2\frac{(r')^3}{r^3} = \frac{y'}{y} = \frac{1}{2} \implies r' = \frac{r}{\sqrt{2}}.
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